The absence of vacuum transition of instantons at temperatures near the electroweak phase transition temperature was invoked in the "sphaleron" interaction to explain the formation of these particles. Isospin, strangeness, and a variable which is defined to be 1 for these particles is related to the charge of the particle, according to the Gell-Mann-Nishijima formula. Any theory which seeks to explain the observed (*) asymmetry in these particles
The absence of vacuum transition of instantons at temperatures near the electroweak phase transition temperature was invoked in the "sphaleron" interaction to explain the formation of these particles. Isospin, strangeness, and a variable which is defined to be 1 for these particles is related to the charge of the particle, according to the Gell-Mann-Nishijima formula. Any theory which seeks to explain the observed (*) asymmetry in these particles and their antiparticles requires the absence of thermal equilibrium, the violation of charge parity symmetry, and the violation of a namesake property according to the Sakharov conditions.  For 10 points, identify these strongly interacting particles which are composed of three quarks, and include neutrons and protons.
The absence of vacuum transition of instantons at temperatures near the electroweak phase transition temperature was invoked in the "sphaleron" interaction to explain the formation of these particles.
{baryons}